WM Paper 5.pdf

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the BoltzmannConstant7
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November15, 2013
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By using a diode we were uUf.ftp construct a circuit from which we measureddifierent voltages. Flom these measurements we were able io
he value of the Boltzmann
constant
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Theory
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In this exlerimelwe measuredthe valueof the Boltzmann
^rrby
$n
ideal diodeequation11]
|
,./a0od
I : Io(""v/ktT- r). .z
,
using the Shockley
(i)
\"/ Jaact
,
This a.llowedus to relate the current through the diode to the voltage acrosst\yi{ode.
In
i. *n" current though the diode, 1o is the reversesaturation current, e is the
this equatiorfi
-v
fundamental element of cha,rge, I/ is the voltage across lhe diode,, 7 is
i the temperature inside
.//'"r/
7{tne
diode,andksis the Boltzmannff.nstant
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m*ti',nt1n ouutor
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Cuu{c(t'L
Method
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we
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JWe measured the voltage at two different points in the circuit (Fig. 1) using a Hewlett Packard
an uncertaintvof + 0.005V.By meaMult'i,meter
972A which gaveour voltagemeasurements
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figu'e.
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avtaxt
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lowcan
suring ihe voltdg6 at two points we were able to indirectly measurethe voltaqe
1;'
i c'-+1
\dAr.,'. a,nd
crrrrent through
throush the
the tr9(tot
trail#tor.
the current
andthe
ttuffitor,
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mdirectly
. t
measured the voltage across the @i"€q[ya
--;V
-:---
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tk fihni,su(
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ryrdss the
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Bv measurinethe voltase utYoint f'lw"
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jwittr respect to groundby-bhranrsee'f-
?rfi nt ; t c@t t1
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-vt. "'i )'r|*rr",i' ,,,,/r';i' vlrf&
t/
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Ot'Lrre&"
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':
, s b/4 f 'kt*4 of l o''^t A
had to usea LF356 op-ampcurrentTo measuretne@d6'W.frrough the transistor uli{*
/.
e 7,
voltageconverterbecausethis curryllli,trmall. This madeit possibleto havea readablevoltage. WA-A{
By measuringthe voltageat point B,Vs,we wereableto indirectlymeasurethe currentthrough ,:O::
::'*n*,
:f^*c'szamqc4,
by using
thetransistor
1r,
uYrtrc{-
t"$i{yA
V:
fi
,^,pryc,sc*Xi'"
o''"f':'u:""ii'*'t
90"1
of the 1 ko pot. L{lke*;5 ,rpr*,#
ffi*{<c.ge alteredtheresistance
We also assumed that the voltage across the diode will make
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)>
1 so we were able to
-t":
approximatethe current through the diode t":?
,
I x loeev/keT .
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2
:t;ry#,
tk
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Vo(.{c,gZtan,^d*f
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We are able to assumethis by starting out measuredvoltageat point A at approximately-0.6V.
From this we can seethat the current will be on the ora", of b)@Junicn
make this approximation valid. F}om this we obtained m#
"
thevottage
v:
LnI:#-tfgr".
rnship betweenl6yI and
r\ttn_>ltrj,,I .
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this'
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We measuredthe resistorRl to be g.gg7+0.002 kfl usinga Stanford,ReaserchSR 7115meter.
1V,tk,/; {,{{/s:;t ,t(;i{rrr,.z-,
,/
PB-503"Protoboard"C'ircu'it
We createdthe circuit ona GlobalSpeci,alti,es
Boardy![&,gna]_y'lit:k-,/*,q
t/r-t
Generator and used BNC Coaci,alCables to connect the multimeter's to the Protoboard. We
LrlL,tltr*,
. ^ - * 't-
rgnoredthe resistancean4 c4ficrtance of the BNC cablgr"cables.During the experimentwe
v,'
v
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,:;i.,-ti,,r
,r4Vq"'
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used a 2NSg04 transistor instead of a diode and assumedthE transiAtoi''would act as a perfect
F'z
tl'r;,
(d:/''
-._--i
-_--j
-l/,u
1rr.t,.:,/,:5.,1
would stay under f .),.,;,, la,; ;.v-1,of thesevoltagesw to n{}ne
W**#E-u#*"ururements
l/
tvt'lpf y',ft':1ri
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t
rl ft;a l-*,
the saturationvoltage.
,!-t l,' ,,/ t-t -'"
i:;gt Ltyt )'( {v|'i'1/v1v' 7:f'4La7ir
-''
/
We made the assumptionthat the temperatureinsideof the transistorwill be approximately
diode. We
: I i n'''
fir1rilV'r.
J(
equalto room temperaturf],rri"t we havemeasured
ro u"d+ - 0.5 K usinga mercuryther,),"'l/t'^
'url
U
f,u
d.. . , . .!l ,.,t+,,
/
trbZ
i
;
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r
!
',1t,''''|u\t,r1'l'.".mometer.ThevoItag.ru'"ntheop_ampwaSmeaSu,"t}+.os+0.005Vand.ftlo,"+ryyLin./
,ti,,,,\
L,i t*'J
flrt
w
tnevoltage
gi1t1ial5fffiand
" ; + 0,005v. Wealso * i), i,' l,/ik:I\
to be -14.94
thecircuitwasmeasur.ed
nl+ry^ui, assumedtheelementoffundamentalchargeetobeexactlyl.64xl0-1eCl3].
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:,if.= ]Co(-
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,
t"t'(l'u"t'rtr:/.*
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f
f
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y. ^.
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we expectedin Eqn. 5. The SravI;fT\8. 2 is a semi-logplot of the current through the diode I
._
='' dt'zt / /rr,
versusthe voltageacrosstrre {$r.d. We wereable to plot the data in Matlab using the program
Y
Flom the measurement,-JdL,"*" fopnd that the relationshipbetween tgql and,Vvrur'lin"ui u,
i, , , ,
5t
,j(
T'l
,
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Boltzmann co\gbdnt. The/reducel ch'i-squaredof our measurementsis 874.88. Our measured
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- ll'L;
wtwlt"n"{ \''c
lYtwt
Lt
c'Botrr*unn
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i)< 10-'J J/K. The known
r.r,o''rrvalue
rr.ll".
constant,kB-"*., wasmeasured
t" b"(;;1+'0.,i6)"lo3?'liN"i'rr"
(i,ttlo,a6)
(
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1-**-**e
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lt-ls
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t }'4k',r,'at' i t"'{t"@t*'( Ls
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hl fi$":"l/" '
trf't5 't4L*"e'1r'|a''tat
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1,,*r,{t,i,,, ,'i
t),;'.ult
4k:
i )
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tlna( 4 t*
is rzez-.ta
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I Figure 2: Semi-logplot of Current versusVol
41.103x+-34.1056
ds,F.1_988q
delb= 1^2847
-*
of the Boltzmann constantis ,be:l3aT1O-23 J lKlS]. Although the value for the known value
\)gtnute
ev are both on the same
^
v{uY of the Boltzmann constant does not lav within our
*,tei,in
discrepancyis most likely due to only havetwo significantfiguresfor
ggggt$acsitudg-This
,.4n1,r,&':'4
the voltagesmeasuredwhich causedus to have multiple data points for one uortage./-i''it;''''''
Su r ' * '
., , I
i''"dyp-
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vt,hi;tnr'lhyq ci*4* 1"t)'4 ?
C [. (tle- tl*lnhrn
'= ()' i 7 7 /]1d/t4
t rlrt J'ii lpa''t (rnuf
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References
sr'^&" Sle! pos)*'*e. ,: /n-v
+- ,-f^"(t''"e
con rLs2ayt^
[1] A. Sedra,K. Smith: MicroelectronicCircuits. 4th ed. New York, New York: Oxford, 1998.
p132-134
\
'/ /
[2] J. Lockhart, W. Man:
{t n,-at;y
Pur(
Advanced Lab l- Manual and S-upplementary information.
Version
F13, San Flancisco,CA: San FlanciscoState University 2013.p76-82
[3] R. Eisberg,R. Resnick: Quantum Physicsof Atoms, Molecules,Solids,Nuclei, and Particles,2nd ed. United State of America: John Wiley & Sons,Inc. 1985.
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